Simulation and scaling analysis of periodic surfaces with small-scale roughness in turbulent Ekman flow

IF 3.6 2区 工程技术 Q1 MECHANICS
Jonathan Kostelecky, Cedrick Ansorge
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The packing density is approximately <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline2.png\"/> <jats:tex-math>$10\\,\\%$</jats:tex-math> </jats:alternatives> </jats:inline-formula> and the roughness elements have a mean height in wall units of <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline3.png\"/> <jats:tex-math>$10 \\lesssim H^+ \\lesssim 40$</jats:tex-math> </jats:alternatives> </jats:inline-formula>. According to their roughness Reynolds numbers, the cases are transitionally rough, although the roughest case is on the verge of being fully rough. We derive the friction of velocity and of the passive scalar through vertical integration of the respective balances. Thereby, we quantify the enhancement of turbulent activity with increasing roughness height and find a scaling for the friction Reynolds number that is verified up to <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline4.png\"/> <jats:tex-math>$Re_\\tau \\approx 2700$</jats:tex-math> </jats:alternatives> </jats:inline-formula>. The higher level of turbulent activity results in a deeper logarithmic layer for the rough cases and an increase of the near-surface wind veer in spite of higher <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline5.png\"/> <jats:tex-math>$Re_\\tau$</jats:tex-math> </jats:alternatives> </jats:inline-formula>. We estimate the von Kármán constant for the horizontal velocity <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline6.png\"/> <jats:tex-math>$\\kappa _{m}=0.42$</jats:tex-math> </jats:alternatives> </jats:inline-formula> (offset <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline7.png\"/> <jats:tex-math>$A=5.44$</jats:tex-math> </jats:alternatives> </jats:inline-formula>) and for the passive scalar <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline8.png\"/> <jats:tex-math>$\\kappa _{h}=0.35$</jats:tex-math> </jats:alternatives> </jats:inline-formula> (offset <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline9.png\"/> <jats:tex-math>$\\mathbb {A}=4.2$</jats:tex-math> </jats:alternatives> </jats:inline-formula>). We find an accurate collapse of the data under the rough-wall scaling in the logarithmic layer, which also yields a scaling for the roughness parameters <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline10.png\"/> <jats:tex-math>$z$</jats:tex-math> </jats:alternatives> </jats:inline-formula>-nought for momentum (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline11.png\"/> <jats:tex-math>$z_{0{m}}$</jats:tex-math> </jats:alternatives> </jats:inline-formula>) and the passive scalar (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0022112024005421_inline12.png\"/> <jats:tex-math>$z_{0{h}}$</jats:tex-math> </jats:alternatives> </jats:inline-formula>).","PeriodicalId":15853,"journal":{"name":"Journal of Fluid Mechanics","volume":"11 1","pages":""},"PeriodicalIF":3.6000,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Fluid Mechanics","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1017/jfm.2024.542","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MECHANICS","Score":null,"Total":0}
引用次数: 0

Abstract

Roughness of the surface underlying the atmospheric boundary layer causes departures of the near-surface scalar and momentum transport in comparison with aerodynamically smooth surfaces. Here, we investigate the effect of $56\times 56$ homogeneously distributed roughness elements on bulk properties of a turbulent Ekman flow. Direct numerical simulation in combination with an immersed boundary method is performed for fully resolved, three-dimensional roughness elements. The packing density is approximately $10\,\%$ and the roughness elements have a mean height in wall units of $10 \lesssim H^+ \lesssim 40$ . According to their roughness Reynolds numbers, the cases are transitionally rough, although the roughest case is on the verge of being fully rough. We derive the friction of velocity and of the passive scalar through vertical integration of the respective balances. Thereby, we quantify the enhancement of turbulent activity with increasing roughness height and find a scaling for the friction Reynolds number that is verified up to $Re_\tau \approx 2700$ . The higher level of turbulent activity results in a deeper logarithmic layer for the rough cases and an increase of the near-surface wind veer in spite of higher $Re_\tau$ . We estimate the von Kármán constant for the horizontal velocity $\kappa _{m}=0.42$ (offset $A=5.44$ ) and for the passive scalar $\kappa _{h}=0.35$ (offset $\mathbb {A}=4.2$ ). We find an accurate collapse of the data under the rough-wall scaling in the logarithmic layer, which also yields a scaling for the roughness parameters $z$ -nought for momentum ( $z_{0{m}}$ ) and the passive scalar ( $z_{0{h}}$ ).
埃克曼湍流中具有小尺度粗糙度的周期性表面的模拟和缩放分析
与空气动力学光滑表面相比,大气边界层下表面的粗糙度会导致近表面标量和动量传输的偏离。在这里,我们研究了 56 次 56 元均匀分布的粗糙度元素对湍流埃克曼流体质的影响。结合沉浸边界法对完全解析的三维粗糙度元素进行了直接数值模拟。堆积密度约为 $10\,\%$,粗糙度元素以壁为单位的平均高度为 $10 \lesssim H^+ \lesssim 40$。根据其粗糙度雷诺数,这些情况都是过渡粗糙,尽管最粗糙的情况濒临完全粗糙。我们通过对各自的平衡进行垂直积分,得出了速度和被动标量的摩擦力。因此,我们量化了湍流活动随粗糙度高度增加而增强的情况,并找到了摩擦雷诺数的缩放比例,该比例最高可达 $Re_\tau \approx 2700$。更高水平的湍流活动导致粗糙度情况下的对数层更深,并且尽管Re_\tau$更高,近表面风偏也会增加。我们估算了水平速度 $\kappa _{m}=0.42$ (偏移 $A=5.44$)和被动标量 $\kappa _{h}=0.35$ (偏移 $\mathbb {A}=4.2$ )的冯卡尔曼常数。我们发现在对数层的粗糙壁缩放下,数据会发生精确的坍缩,这也产生了动量($z_{0{m}}$)和被动标量($z_{0{h}}$)的粗糙度参数$z$-无缩放。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
6.50
自引率
27.00%
发文量
945
审稿时长
5.1 months
期刊介绍: Journal of Fluid Mechanics is the leading international journal in the field and is essential reading for all those concerned with developments in fluid mechanics. It publishes authoritative articles covering theoretical, computational and experimental investigations of all aspects of the mechanics of fluids. Each issue contains papers on both the fundamental aspects of fluid mechanics, and their applications to other fields such as aeronautics, astrophysics, biology, chemical and mechanical engineering, hydraulics, meteorology, oceanography, geology, acoustics and combustion.
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